Systematic measurement of pd breakup cross section at quasi-free scattering Y. Eguchi a, K. Sagara...
-
Upload
adeline-allread -
Category
Documents
-
view
212 -
download
0
Transcript of Systematic measurement of pd breakup cross section at quasi-free scattering Y. Eguchi a, K. Sagara...
Systematic measurement of pd breakupcross section at quasi-free scattering
Y. Eguchia, K. Sagaraa, S. Kuroitaa, K. Yashimaa,
T. Shishidoa, T. Yabea, and S. Ishikawab
aDepartment of Physics, Kyushu UniversitybDepartment of Physics, Science Research Center, Hosei University
31 August 2009 19th International IUPAP Conference on Few-Body Problems in Physics 2
Discrepancies in 3N system
3N binding energyproblem
1980’s
3NF(FM) was found
1998 pd captureAjj discrepancy
pd breakupdiscrepancy
3NF ?3NF ?
Relativity ?
① Higher energy discrepancies
pd elastic scatt.discrepancy
② Lower energy discrepancies
Space Star AnomalyQuasi-Free Scatt. Anomaly ?
???
FM-3NF1957
pd elastic scatt.C.S. discrepancy
1994-1996-1997
Ay puzzle1986
Ay puzzle ???
Space Star Anomaly1989
N N N
π
π
N N N
πρ
Space Star (SS) Anomaly
• SS Anomaly was first found in 1989 in nd breakup reaction at 13 MeV.
31 August 2009 19th International IUPAP Conference on Few-Body Problems in Physics 3
Space Star(c.m. system)
equilateral triangle
90°
nd exp. Erlangen & TUNL(●) (○)
nd calc.
Space Star
(1989) (1996)
J.STRATE et al., Nucl. Phys. A501 (1989) 51H.R.Setze et al., Physics Letters B388 (1996) 229G.RAUPRICH et al., Nucl. Phys. A535 (1991) 313
pd exp.Koeln ( 1991 )
EN=13 MeV
~30%
• In Star configuration, outgoing 3 nucleons have the same energy and form an equilateral triangle.
• In Space Star (SS), the star plane is perpendicular to the beam axis in c.m. system.
Space Star (SS) Anomaly in pd breakup
• Recently pd calc. have become available (by Deltuva et al. and by Ishikawa).
31 August 2009 19th International IUPAP Conference on Few-Body Problems in Physics 4
nd calc.
pd calc. by Deltuva et al. (2005)
pd exp.Koeln (□) & KUTL
(■)
A.Deltuva et al., PRC72,054004 (2005)
(2002)
EN=13 MeV nd exp. Erlangen & TUNL(●) (○)
nd calc.
Space Star
(1989) (1996)
pd exp.Koeln ( 1991 )
EN=13 MeV
~30%
~15%
• At pd SS, exp. cross section is smaller than pd calc.
• At nd SS, exp. cross section is larger than nd calc.
Energy dependence of SS Anomaly
• SS Anomaly has a maximum at around EN = 13 MeV.
31 August 2009 19th International IUPAP Conference on Few-Body Problems in Physics 5
Erlangen
ErlangenBochumTUNL
TUNL
TUNL
Koeln
Koeln
Koeln
KUTL
Space Star
G. Rauprich et al., Nucl. Phys. A 535, 313 (1991).G. Grossmann et al., Nucl. Phys. A 603, 161 (1996).H. Patberg et al., Phys. Rev. C 53, 1497 (1996).K. Gebharbt et al., Nucl. Phys. A 561, 232 (1993).H. R. Setze et al., Phys. Lett. B 388, 229 (1996).Z. Zhou et al., Nucl. Phys. A 684, 545 (2001).M. Stephan et al., Phys. Rev. C 39, 2133 (1989).
90°
p + d
n + d~30%
~15%
Off-plane Star
• An angle between the star plane and the beam axis in c.m. system is defined as an inclined angle α.
– α = 90 deg. at Space Star
31 August 2009 19th International IUPAP Conference on Few-Body Problems in Physics 6
Off-plane Star(c.m. system)
• Systematic measurements of pd breakup cross section have been started
at Off-plane Star
in 0° ≦ α ≦ 180 °
at Ep = 9.5 MeV (Ed = 19 MeV) and Ep = 13 MeV (Ed = 26 MeV).
α
・ Anomaly exists at forward angles. → My talk
• Star Anomaly has different α dependence between
9.5 MeV and 13 MeV. → Maeda’s talk (nuclear forces session)
dependence of Star Anomaly
31 August 2009 19th International IUPAP Conference on Few-Body Problems in Physics 7
Space Star (α = 90 deg.)
α=144º
α=124º
J. Ley et al, (Koeln) PRC73 (2006) 064001
EN=13 MeV
~15%
Discrepancy at Quasi-free Scattering
• At forward angles, star configuration is close to Quasi-free Scattering (QFS) configuration.
• Cross section become several times larger than SS cross section.
• Therefore, the anomaly at forward angles, is considered to be QFS anomaly than Star Anomaly.
31 August 2009 19th International IUPAP Conference on Few-Body Problems in Physics 8
~ QFS~ QFS
~ QFS~ QFS
En
Space Star (α = 90 deg.)
90°
α = 0 deg.
QFS condition
31 August 2009 19th International IUPAP Conference on Few-Body Problems in Physics 9
p + d → p1 + p2 + n
QFSQFS
Star =0°Star =0° QFS
We measure pd breakup C.S. at QFS configuration.
Experiment (pp-QFS) p-beam : Ep=9.5 MeV, 13 MeV (~150 nA) @ KUTL
Target : CD2 foil (thickness : ~0.3mg/cm2)
Detector : Si-SSD (solid angle : ~0.4 msr)
Observable : cross section
Target thickness was monitored by using pd elastic scattering.
We used accurate pd elastic C.S. to obtain absolute pd breakup C.S..
31 August 2009 19th International IUPAP Conference on Few-Body Problems in Physics 10
p-beam F.C.
Si-SSD
CD2 foil
CD2 foil (Rotary target)
M
Monitor
K. Sagara et al., Phys. Rev. C 50, 576 (1994)
dSdd
d
21
3
Data analysis• We measure Energy and Time of Flight of 2 proton.
31 August 2009 19th International IUPAP Conference on Few-Body Problems in Physics 11
TOF
gate
background
TOF gate
E1 vs. E2
ΔT2-ΔT1 vs. ΔT (E2,E1)
E1 vs. E2
background
E1 vs. E2
B.G. subtracted
S curve
Raw data
TOF data
Result (pp-QFS)
31 August 2009 19th International IUPAP Conference on Few-Body Problems in Physics 12
QFSQFS
Ep= 9.5 MeV Ep= 13 MeV
QFSQFS
~10% smaller~10% smaller ~13% smaller~13% smaller
Energy dependence of QFS Anomaly
31 August 2009 19th International IUPAP Conference on Few-Body Problems in Physics 13
Ep= 9.5 MeV
Ep= 13 MeV
QFS
KUTL
Bochum ( 1992 )
( )
10 ~ 13%
p + d
n + d
~10%
~13%
Energy dependence of QFS Anomaly
31 August 2009 19th International IUPAP Conference on Few-Body Problems in Physics 14
A. Siepe et al., Phys. Rev. C 65, 034010 (2002)
X. C. Ruan et al., Phys. Rev. C 75, 057001 (2007)
Bonn univ.( 2002 )En=26 MeV
CIAE ( 2007 )En=25 MeV
~ 18%
θ1= θ2= 42 deg.
θ1= θ2= 42.2 deg.
~ 16%
QFS
KUTL
Bochum ( 1992 )
( )
10 ~ 13%
p + d
n + d
16 ~ 18%
Energy dependence of QFS Anomaly
31 August 2009 19th International IUPAP Conference on Few-Body Problems in Physics 15
~30%
~15%
Space Star
90°
p + d
n + d
QFS
KUTL
Bochum ( 1992 )
( )
10 ~ 13%
p + d
n + d
16 ~ 18%
Large charge asymmetry
Systematic measurement of C.S. at around QFS
31 August 2009 19th International IUPAP Conference on Few-Body Problems in Physics 16
QFSQFS
Ep= 9.5 MeV Ep= 13 MeV
θ1 = θ2θ1 = θ2 θ1 = θ2
θ1 = θ2
Star α=0
QFSQFS
Star α=0
p + d → p1 + p2 + n
Angle dependence of QFS Anomaly
31 August 2009 19th International IUPAP Conference on Few-Body Problems in Physics 17
①②③④ ⑤ ⑥ ⑦
1
5
4
23
Ep= 9.5 MeV
Ep= 13 MeV
6
7 1 42 3 5 46 7
① ② ③
QFS (9.5 MeV)QFS (9.5 MeV) θ1 = θ2 (9.5 MeV)θ1 = θ2 (9.5 MeV)
QFS 13 MeVQFS 13 MeV θ1 = θ2 13 MeVθ1 = θ2 13 MeV
~10 %
~ 15%
Summary
• We performed systematic measurement of pd breakup cross section at around Quasi-free Scattering (QFS).
• Those experimental results were compared with the calculation included coulomb force by Deltuva et al..
• Both at 9.5 MeV and 13 MeV ,
pd experimental data are smaller than pd calculation generally.
• Large charge asymmetry was found both in SS Anomaly and in QFS Anomaly;
experiment > calculation at nd breakup and
experiment < calculation at pd breakup.
• We will continue systematic experiment of pd breakup cross section
to find the origin of Star Anomaly and QFS Anomaly.
31 August 2009 19th International IUPAP Conference on Few-Body Problems in Physics 18
31 August 2009 19th International IUPAP Conference on Few-Body Problems in Physics 19
31 August 2009 19th International IUPAP Conference on Few-Body Problems in Physics 20
Discrepancies in 3N system
3N binding energyproblem
1980’s
3NF(FM) was found
1998 pd captureAjj discrepancy
pd breakupdiscrepancy
3NF ?3NF ?
Relativity ?
① Higher energy discrepancies
pd elastic scatt.discrepancy
② Lower energy discrepancies
Space Star AnomalyQuasi-Free Scatt. Anomaly
???
FM-3NF1957
pd elastic scatt.C.S. discrepancy
1994-1996-1997
Ay puzzle1986
Ay puzzle ???
Space Star Anomaly1989
N N N
π
π
N N N
πρ
Space Star (SS)
• In Star configuration, outgoing 3 nucleons have the same energy and form an equilateral triangle.
• In Space Star (SS), the star plane is perpendicular to the beam axis in c.m. system.
• Star configuration is most far from Final State Interaction (FSI) configuration.– In FSI configuration, one of relative energy = 0.– FSI enhances Cross Section.
• It is expected that small effects are seen in Star configuration.
31 August 2009 19th International IUPAP Conference on Few-Body Problems in Physics 21
Space Star(c.m. system)
equilateral triangle
90°FSI
pd
Relative energy = 0